Implications of N $$ \mathcalN} $$ = 5, 6 superconformal symmetry in three spacetime dimensions

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Location: Deutsche Nationalbibliothek Frankfurt am Main

ISSN: 1029-8479

Extent: Online-Ressource

Language: Englisch

Notes: online resource.

Bibliographic citation: Implications of N $$ \mathcalN} $$ = 5, 6 superconformal symmetry in three spacetime dimensions ; volume:2016 ; number:8 ; day:11 ; month:8 ; year:2016 ; pages:1-24 ; date:8.2016
Journal of high energy physics ; 2016, Heft 8 (11.8.2016), 1-24, 8.2016

Creator: Kuzenko, Sergei M.

Contributor: Samsonov, Igor B.
SpringerLink (Online service)

DOI: 10.1007/JHEP08(2016)084

URN: urn:nbn:de:1111-2016090930390

Rights: Der Zugriff auf das Objekt ist unbeschränkt möglich.

Last update: 14.08.2025, 11:03 AM CEST

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Kuzenko, Sergei M.
Samsonov, Igor B.
SpringerLink (Online service)

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Bootstrapping N = 3 $$ \mathcalN}=3 $$ superconformal theories

$The N = 2 $$ \mathcalN}=2 $$ superconformal bootstrap$

The N = 2 $$ \mathcalN}=2 $$ superconformal bootstrap

$Revisiting N = 4 $$ \mathcalN}=4 $$ superconformal blocks$

Revisiting N = 4 $$ \mathcalN}=4 $$ superconformal blocks

$Four-dimensional $$\mathcalN}$$ = 2 superconformal long circular quivers$

Four-dimensional $$\mathcalN}$$ = 2 superconformal long circular quivers

$Reviving 3D N $$ \mathcalN} $$ = 8 superconformal field theories$

Reviving 3D N $$ \mathcalN} $$ = 8 superconformal field theories

$Towards N $$ \mathcalN} $$ = 2 superconformal higher-spin theory$

Towards N $$ \mathcalN} $$ = 2 superconformal higher-spin theory

$Chiral correlators in N $$ \mathcalN} $$ = 2 superconformal quivers$

Chiral correlators in N $$ \mathcalN} $$ = 2 superconformal quivers

$New N $$ \mathcalN} $$ = 2 superconformal field theories from S $$ \mathcalS} $$ -folds$

New N $$ \mathcalN} $$ = 2 superconformal field theories from S $$ \mathcalS} $$ -folds

$Mixed OPEs in N = 2 $$ \mathcalN}=2 $$ superconformal theories$

Mixed OPEs in N = 2 $$ \mathcalN}=2 $$ superconformal theories

$Wilson loop correlators in N $$ \mathcalN} $$ = 2 superconformal quivers$

Wilson loop correlators in N $$ \mathcalN} $$ = 2 superconformal quivers

$N $$ \mathcalN} $$ = 4 superconformal bootstrap of the K3 CFT$

N $$ \mathcalN} $$ = 4 superconformal bootstrap of the K3 CFT

$Implications of N=4 $$ \mathcalN}=4 $$ superconformal symmetry in three spacetime dimensions$

Implications of N=4 $$ \mathcalN}=4 $$ superconformal symmetry in three spacetime dimensions

$Bootstrapping N = 3 $$ \mathcalN}=3 $$ superconformal theories$

Bootstrapping N = 3 $$ \mathcalN}=3 $$ superconformal theories

$The N = 2 $$ \mathcalN}=2 $$ superconformal bootstrap$

The N = 2 $$ \mathcalN}=2 $$ superconformal bootstrap

$Revisiting N = 4 $$ \mathcalN}=4 $$ superconformal blocks$

Revisiting N = 4 $$ \mathcalN}=4 $$ superconformal blocks

$Four-dimensional $$\mathcalN}$$ = 2 superconformal long circular quivers$

Four-dimensional $$\mathcalN}$$ = 2 superconformal long circular quivers

$Reviving 3D N $$ \mathcalN} $$ = 8 superconformal field theories$

Reviving 3D N $$ \mathcalN} $$ = 8 superconformal field theories

$Towards N $$ \mathcalN} $$ = 2 superconformal higher-spin theory$

Towards N $$ \mathcalN} $$ = 2 superconformal higher-spin theory

$Chiral correlators in N $$ \mathcalN} $$ = 2 superconformal quivers$

Chiral correlators in N $$ \mathcalN} $$ = 2 superconformal quivers

$New N $$ \mathcalN} $$ = 2 superconformal field theories from S $$ \mathcalS} $$ -folds$

New N $$ \mathcalN} $$ = 2 superconformal field theories from S $$ \mathcalS} $$ -folds

$Mixed OPEs in N = 2 $$ \mathcalN}=2 $$ superconformal theories$

Mixed OPEs in N = 2 $$ \mathcalN}=2 $$ superconformal theories

$Wilson loop correlators in N $$ \mathcalN} $$ = 2 superconformal quivers$

Wilson loop correlators in N $$ \mathcalN} $$ = 2 superconformal quivers

$N $$ \mathcalN} $$ = 4 superconformal bootstrap of the K3 CFT$

N $$ \mathcalN} $$ = 4 superconformal bootstrap of the K3 CFT

$Implications of N=4 $$ \mathcalN}=4 $$ superconformal symmetry in three spacetime dimensions$

Implications of N=4 $$ \mathcalN}=4 $$ superconformal symmetry in three spacetime dimensions

$Bootstrapping N = 3 $$ \mathcalN}=3 $$ superconformal theories$

Bootstrapping N = 3 $$ \mathcalN}=3 $$ superconformal theories

$The N = 2 $$ \mathcalN}=2 $$ superconformal bootstrap$

The N = 2 $$ \mathcalN}=2 $$ superconformal bootstrap

$Revisiting N = 4 $$ \mathcalN}=4 $$ superconformal blocks$

Revisiting N = 4 $$ \mathcalN}=4 $$ superconformal blocks

$Four-dimensional $$\mathcalN}$$ = 2 superconformal long circular quivers$

Four-dimensional $$\mathcalN}$$ = 2 superconformal long circular quivers

$Reviving 3D N $$ \mathcalN} $$ = 8 superconformal field theories$

Reviving 3D N $$ \mathcalN} $$ = 8 superconformal field theories

$Towards N $$ \mathcalN} $$ = 2 superconformal higher-spin theory$

Towards N $$ \mathcalN} $$ = 2 superconformal higher-spin theory

$Chiral correlators in N $$ \mathcalN} $$ = 2 superconformal quivers$

Chiral correlators in N $$ \mathcalN} $$ = 2 superconformal quivers

$New N $$ \mathcalN} $$ = 2 superconformal field theories from S $$ \mathcalS} $$ -folds$

New N $$ \mathcalN} $$ = 2 superconformal field theories from S $$ \mathcalS} $$ -folds

$Mixed OPEs in N = 2 $$ \mathcalN}=2 $$ superconformal theories$

Mixed OPEs in N = 2 $$ \mathcalN}=2 $$ superconformal theories

$Wilson loop correlators in N $$ \mathcalN} $$ = 2 superconformal quivers$

Wilson loop correlators in N $$ \mathcalN} $$ = 2 superconformal quivers

$N $$ \mathcalN} $$ = 4 superconformal bootstrap of the K3 CFT$

N $$ \mathcalN} $$ = 4 superconformal bootstrap of the K3 CFT

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Implications of N $$ \mathcalN} $$ = 5, 6 superconformal symmetry in three spacetime dimensions

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Other Objects (12)

Implications of N=4 $$ \mathcalN}=4 $$ superconformal symmetry in three spacetime dimensions

Bootstrapping N = 3 $$ \mathcalN}=3 $$ superconformal theories

The N = 2 $$ \mathcalN}=2 $$ superconformal bootstrap

Revisiting N = 4 $$ \mathcalN}=4 $$ superconformal blocks

Four-dimensional $$\mathcalN}$$ = 2 superconformal long circular quivers

Reviving 3D N $$ \mathcalN} $$ = 8 superconformal field theories

Towards N $$ \mathcalN} $$ = 2 superconformal higher-spin theory

Chiral correlators in N $$ \mathcalN} $$ = 2 superconformal quivers

New N $$ \mathcalN} $$ = 2 superconformal field theories from S $$ \mathcalS} $$ -folds

Mixed OPEs in N = 2 $$ \mathcalN}=2 $$ superconformal theories

Wilson loop correlators in N $$ \mathcalN} $$ = 2 superconformal quivers

N $$ \mathcalN} $$ = 4 superconformal bootstrap of the K3 CFT

Implications of N=4 $$ \mathcalN}=4 $$ superconformal symmetry in three spacetime dimensions

Bootstrapping N = 3 $$ \mathcalN}=3 $$ superconformal theories

The N = 2 $$ \mathcalN}=2 $$ superconformal bootstrap

Revisiting N = 4 $$ \mathcalN}=4 $$ superconformal blocks

Four-dimensional $$\mathcalN}$$ = 2 superconformal long circular quivers

Reviving 3D N $$ \mathcalN} $$ = 8 superconformal field theories

Towards N $$ \mathcalN} $$ = 2 superconformal higher-spin theory

Chiral correlators in N $$ \mathcalN} $$ = 2 superconformal quivers

New N $$ \mathcalN} $$ = 2 superconformal field theories from S $$ \mathcalS} $$ -folds

Mixed OPEs in N = 2 $$ \mathcalN}=2 $$ superconformal theories

Wilson loop correlators in N $$ \mathcalN} $$ = 2 superconformal quivers

N $$ \mathcalN} $$ = 4 superconformal bootstrap of the K3 CFT

Implications of N=4 $$ \mathcalN}=4 $$ superconformal symmetry in three spacetime dimensions

Bootstrapping N = 3 $$ \mathcalN}=3 $$ superconformal theories

The N = 2 $$ \mathcalN}=2 $$ superconformal bootstrap

Revisiting N = 4 $$ \mathcalN}=4 $$ superconformal blocks

Four-dimensional $$\mathcalN}$$ = 2 superconformal long circular quivers

Reviving 3D N $$ \mathcalN} $$ = 8 superconformal field theories

Towards N $$ \mathcalN} $$ = 2 superconformal higher-spin theory

Chiral correlators in N $$ \mathcalN} $$ = 2 superconformal quivers

New N $$ \mathcalN} $$ = 2 superconformal field theories from S $$ \mathcalS} $$ -folds

Mixed OPEs in N = 2 $$ \mathcalN}=2 $$ superconformal theories

Wilson loop correlators in N $$ \mathcalN} $$ = 2 superconformal quivers

N $$ \mathcalN} $$ = 4 superconformal bootstrap of the K3 CFT

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